ANALYSIS OF HEART WAVE FORMS

Abstract: A method of analysing Ventricular Late Potential (VLP) including determining a parameter related to the complexity of the VLP as a parameter for clinical evaluation. The method may include computing the fractal dimension of the attractor for the VLP as a parameter for clinical evaluation. The method may include performing a spectral analysis producing an assessment based on a discrete Hartley transform (DHT) vector spectrum by summing amplitude components between -f1 to -f2 and +f2 to +f1, where f1 is a number larger than f2.

Description: ANALYSIS OF HEART HAVEFORMS This invention relates to the analysis of heart waveforms and more particularly to the heart waveform represented by the measurement known as the Ventricular Late Potential (VLP). It is known to apply temporal fractals to the study of cardiac rhythm (Goldberger e_t al. , Experimental 1988; 44: 983-987 and other citations in IEEE Engineering in Medicine and Biology, 1992, June p52). Goldberger suggests that disease states may lead to a loss of the physiological complexity of measurements and therefore to greater regularity, not a greater irregularity, in the measured phenomenon. It is an object of the invention to provide from an analysis of ventricular late potential measurements an indication of a parameter significant for clinical evaluation. The invention provides a method of analysing Ventricular Late Potential (VLP) including determining a parameter related to the complexity of the VLP as a parameter for clinical evaluation. According to the invention there 1s provided a method of analysing Ventricular Late Potential (VLP) including computing the fractal dimension of the attractor for the VLP as a parameter for clinical evaluation. Preferably the VLP attractor is that in three dimensional voltage space, the voltage being ECG measurements. The geometrical realisation of the attractor, which need not be carried out to perform the invention, may be considered as a path in phase space defined by ECG voltages in three orthogonal directions. The method may include an approximation to the fractal dimension of the attractor as the quotient of log(L)/log(DD), where L is the total length of the attractor and DD is the spheric extent diameter of the attractor. The approximation may be produced by the application of an algorithm, conveniently in the form of a flow chart. The method may include assessing the ECG signals to define VLP onset and offset points. The assessment of the ECG signals may include signal-averaging and high-pass filtering and the taking of the absolute value of the filtered output. In one assessment the onset is defined as the vector magnitude combination exceeding a chosen mean or peak voltage. This may be 40 micro volts mean or 48 microvolts peak (mean ± 20%). In one assessment the offset is defined as the mean voltage exceeding the mean noise level plus three times the standard deviation of the noise sample. A fractal dimension in excess of 1.30 may be selected as the value indicating a risk of sudden cardiac death positive (SCD+) condition. The fractal dimension may be provided as a display or other output. To optimise ECG signal collection a particular form of amplifier may be employed including three operational amplifiers with a high gain in an early front end stage to minimise noise over a controlled bandwidth, which may be 0.1 to 1200Hz, and low crosstalk, which may be below -90dB. Spectral analysis of VLP may be performed to produce an assessment based on a dlsrete Hartley transform (DHT) vector spectrum by summing amplitude components between -f 1 to -f 2 and +f£ to +f^ where f ] Is a number larger than f 2 . A value in the upper part of the range of an Individual assessment for a group Including persons believed healthy and persons believed to be SCD+ Indicates risk of SCD+ and provides a parameter for clinical evaluation. The basic fractal techniques are now becoming known from the works of several authors including B.B. Mandelbrodt, J. Feder and D. Stauffer and H.E. Stanley to which reference is directed for these techniques. Embodiments of the invention will now be described with reference to the accompanying drawings, in which: Figure 1 is a diagram of electrode positions on the front, sides and back of a human torso, Figure 2 is a flow chart for an algorithm for computing the fractal dimension of an attractor, Figure 3 shows equations useful in practicing the invention, Figures 4 and 5 are each the representation of an attractor, Figures 6a, 6b, 7 and 8 are tables of results of measurements according to the invention, Figures 9 and 10 each show a DHT vector spectrum, and Figure 11 shows a circuit diagram of an amplifier for ECG signals. Figure 1 shows the position of electrodes in the conventional bipolar orthogonal XYZ lead system. The pairs of electrodes (+X, -X) (+Y, -Y) and (+Z, -Z) each relate to an orthogonal axis, X, Y and Z respectively. Electrode -Z is on the back of the torso, electrode +Z on the front, electrodes +X and -X are on the sides of the torso and electrodes +Y and -Y at the top and bottom respectively of the torso. A reference lead electrode (REF) is also used. Standard, pre-gelled, disposable ECG electrodes are used. For analysis purposes the three channels (X, Y and Z) are recorded simultaneously in digital form. In one arrangement, according to the invention, a low noise, high gain, three channel ECG amplifier having a frequency band width from 0.1 to 1200 Hz and cross talk below -90dB is used for conditioning the ECG signals from electrode pairs. (Figure 11 shows such an amplifier.) Each channel is digitised at 4000 Hz with 16-bit resolution. Each ECG digital recording is 7 or 11 megabytes In length, depending on the basic heart rate and the background noise during the recording. Gain for each channel can be set independently at between 1000 and 20000 and the values noted for the later off-line processing. A back-up record is made on a tape streamer. Off-line signal processing of each ECG is as follows. Signal averaging is performed until the rms noise level during diastole is less than 0.3 microvolts. Standard deviation of trigger jitter is estimated to be less than 0.2 milliseconds, provided that the rms noise level in the raw ECG is less than 40 microvolts. The Single Fiducial Point (SFP) alignment technique is used (Escalona O.J. si 4l. , A fast and reliable beat alignment technique, Med. Bio. Eng & Comp., 29, Supp, 1991). Each beat is cross correlated with a template beat and was rejected for averaging if it was an ectopic beat. Excessively noisy beats with rms noise greater than 40 microvolts are also rejected. High-pass filtering is performed digitally on each signal averaged lead. A 40 Hz bidirectional 4th order Butterworth high-pass filter is used according to the standard method (Breithardt. G. si 4l- Standards for analysing of ventricular late potentials, Eur. Heart 0. (1991) 12, 473-480) to produce signals Xf, Y and If. Analysis 1n accordance with the Invention is carried out on these filtered signals, after taking absolute values of the filter output. Ventricular late potentials (VLP) start and end points are defined as follows. The end point (VLP 0 f) for each signal is defined as the mid-point of a 5 milliseconds segment shifted along the ST segments towards the QRS complex in one millisecond steps until the mean voltage exceeds the mean noise level plus three times the standard deviation of noise sample (see Breithardt, above). The terms QRS and ST are those regularly used for electrocardiograms. The largest value of VLP 0 ff among the three is chosen as the end point ( tg = largest VLP off ). The starting time of the VLP (t ) is defined on the vector magnitude combination of the three filtered orthogonal leads (Xf 2 + Y f 2 + lf 2 ) Vl , as the end-point ("right-hand" end) of a 5 milliseconds segment shifted from t → z into the QRS complex in one millisecond steps until its mean voltage exceeds 40 microvolts or has a peak value of 48 microvolts (i.e. 40 microvolts + 20%) to accommodate very brief peaking of the VLP vector magnitude. All the VLP amplitude values are expressed in microvolt units and the VLP attractor is traced in the three dimensional voltage space with the X, Y, Z leads as the orthogonal axis (μV3D space). (See Figures 4 and 5). Each point of the trace corresponds to a certain time between t 0 and t → z and has as co-ordinates the values of VLP amplitude of each corresponding filtered lead (X, Y, Z) at that particular time. An important feature of the invention is the estimated fractal dimension (δ) of the VLP attractor. A technique for this estimation is described below and uses the following expression: δ = log(L)/log(DD) where L is the total length of the trajectory of the attractor and DD is the spheric extent (maximum diameter) encompassing the attractor (both measured 1n microvolts). The attractor trajectory (see Figures 4 and 5) is a discrete 3D curve in which points correspond to the sampling interval in each ECG lead recording (in one example 0.25 milliseconds). The total length L 1s the sum of all the step distances between adjacent points in the curve. If there are N time steps each of 0.25 milliseconds between t 0 and t^ then L 1s given by Equation 1 1n Figure 3. The maximum diameter DD is obtained as follows. For every one of the N points on the curve the values of distance to each other (N-l) points is calculated. The absolute maximum of all the calculated distances is evaluated. The distance Dij between an 1th and a jth point 1n the attractor curve is given by Equation 2 in Figure 3. The matrix representation of all possible Dij elements, namely the distance matrix Δ, is equation 3 in Figure 3. In theory the determination of DD requires the computation of N*(N-I) distances, i.e. computation of equation (3) for N*(N-1) times. N has been found to be as large as 320 in some abnormal subjects (VLP duration of 80 milliseconds) and thus some 10 4 computations would be needed for DD. However, Dij = Dji, i.e. Δ is symmetrical. Accordingly the number of calculated distances can be halved if the process for DD is carried out on only the distance elements in the upper triangle of Δ. This is expressed as follows: ibed above. Figures 4 and 5 show in convenient projections VLP attractors actually measured 1n accordance with the invention. The values plotted are up to some tens of microvolts. The value of δ calculated as above 1s shown on each Figure. Relating these Figures to Figure 1 the H/T axis (head/feet) corresponds to the +Y/-Y electrodes, the R/L axis (right side/left side) corresponds to the -X/+X electrodes and the F/B axis (torso front/torso back) corresponds to the +Z/-Z electrodes. Figure 4 is the VLP attractor for a person believed to be healthy (δ = 1.1214) and Figure 5 the VLP attractor for a person believed to be SCD+ (that is at risk of Sudden Cardiac Death) (δ «= 1.4373) on the accepted Late Potential prediction criteria (Breithardt e-± al. above). It is widely accepted that certain directly observable Late Potential features are a useful predictor of SCD+ for a person after a myocardial Infraction (MI). Breithardt £± 4l. set these out as three criteria: (1) fQRSd longer than 114 milliseconds (2) RMS40 less than 20 microvolts (3) LAS40 longer than 38 milliseconds (Here fQRSd is the filtered QRS duration, RMS40 is the root mean square amplitude of the terminal 40 millisecond and LAS40 the duration of low amplitude signals (below 40 microvolts) in the vector magnitude QRS complex using 40 Hz high-pass bidirectional filtering.) When at least two of the three criteria are satisfied a person should be considered to be late potential positive (LP+) and if post - MI considered to be SCD+. Figures 6a and 6b show results for a group of 45 persons believed healthy (regardless of whether they presented as normal VLP activity or not, mean age 38 ± 8 years). Figure 7 shows results for a group of 19 persons believed post-MI SCD+ and at risk (according to their medical history and having abnormal VLP activity according to the above standard analysis, mean age 58 ± 12 years). Column P# distinguishes the persons in each group, other columns are the above three conventional criteria while δ is the fractal dimension calculated according to the invention. The Figures include the mean value (MV) and standard deviation (SD). Figure 8 shows the pooled variance (PV) and separated variance (SV) for a statistical Student t-test on the criteria results for the group in Figures 6a and 6b against the criteria results for the group in Figure 7. The conventional criteria (RMS40, LAS40 and fQRSd) referred to above are from the time-domain of the electrode waveforms and depend on the algorithm used for detecting the onset and offset points of the filtered QRS complex. (This algorithm implements a standard definition given in Breithardt for the onset and offset points of the filtered QRS complex.) When micropotentials (less than 5 microvolts) are long delayed and with slow termination the algorithm is expected to err systematically, especially under noisy conditions. By using a parameter defined in the 3-D micro voltage space instead of the 2D voltage-time plane significant advantages are achieved. In the 3-D space curved behaviour depends only on voltage changes. A consequence of this is that small voltage changes (less than 5 microvolts) in a relatively long period of time can yield only small curve changes. Large curve fluctuations or changes would increase the complexity of the curve and consequently its fractal dimension. The fractal dimension method requires the use of the VLP 0 ff detection algorithm but the value of δ is less critically dependent on the performance of the algorithm. The voltage range of ±40 microvolts is specified by the definition of VLP. For smaller ranges, say ± 5 microvolts, the computed values of δ would have been different, more sensitive to sub-microvolt late potential activity and more susceptible to noise after signal averaging. Values of δ ranged between 1 and 1.5 for the technique described above. From the definition of the Hausdorff-Besicovltel dimension δ can not be greater than 3. The value of δ 1s close to 1 when the VLP attractor converges from a +40 or a -40 microvolt potential (at the VLP starting point) to the origin (VLP 0 ff) in a practically straight line trajectory. In the case of subjects believed healthy there 1s a very sharp termination of the QRS complex. The contrast between a VLP attractor trajectory with a δ value closer to 1 (δ=1.1214) and one with a δ value closer to 1.5 (δ=1.4373) is seen from Figures 4 and 5. Apparatus to perform the invention can be arranged in any convenient form. One arrangement is a specific electronic unit to which suitable signals are supplied and which carries out the attractor fractal dimension computation with suitably arranged electronic calculating devices to provide an indication on the unit or an associated display of the calculated fractal dimension for the supplied signals. The ECG signal amplifiers described herein may be associated with or Incorporated 1n the apparatus if required. The size of the sample shown in the tables of results is relatively small but is sufficient for an assessment of the clinical significance of δ as an indicator (discriminator) of SCD+ in patients. Further a threshold value for δ can be identified above by which a post-MI patient can be classified as SCD+. A suggested basis for this value ( ςr j + ) is the mean value of δ in the group of persons believed healthy plus two times the standard deviation (Figure 6). In this specific example this value is 1.337. An alternative suggested basis for such a threshold value is the mean value of δ for the group of persons believed healthy (1.2124) and δ for the group of persons believed to be SCD+ (1.3737), this value of δ SCD+ is 1.293. The justification for this basis is the closeness of the standard deviation of δ for the two groups shown, viz 0.062 and 0.054. A value of δ SC o + of 1.30 produces three false positives in the "healthy" group and one false negative in the "SCD+" group. A canine model study provided more controlled conditions than possible with human patients. (For example in the Figure 6 "healthy" group there are some LP+ conditions while the post-MI group of Figure 7 includes cases which could have become completely healed). This model study yielded smaller and closer deviations for the "healthy" and SCD+ groups (0.0411 and 0.0468 respectively). The smaller deviations reflected the more controlled conditions of the model study. The above techniques show that it is likely that the fractal dimension of the VLP attractor 1n post-MI, SCD+ subjects is significantly higher than in "healthy" subjects, to the degree of 1 part 1n 1000 that this is not the case. Further, compared to the QRS offset detection method, the above technique has a lower vulnerability to errors made by the algorithem and therefore offers better reliability in automated use. The complexity in υ V3D space can be interpreted as a measure of chaotic behaviour that could trigger a catastrophic arrhythimic episode. Figures 9 and 10 show the results of another technique according to an aspect of the invention for assessing VLP in which a discrete Hartley transform vector spectrum is used. The spectrum amplitude components (A) are summed in two frequency ranges, -f^ to -f 2 and +f 2 to +f- j , for example -300Hz to -60Hz and +60Hz to +300 Hz. Figure 9 is an assessment for a person believed healthy and Figure 10 for a person believed SCD+. A higher value in the range of summed components for healthy and SCD+ persons indicates SCD+ risk. The higher value of summed components is believed to relate to increased complexity of the VLP and thus to SCD and condition. Figure 11 is the circuit diagram of an ECG amplifier to enhance signal collection and useful in the practice of the present invention. A three-operational amplifier front end FE has high early gain to minimise noise over a controlled bandwidth, for example 0.1 to 1200Hz and low crosstalk, below -90dB. The amplifier for only one electrode pair, for example the x axis +E χ and -E x supplying one channel X is shown for simplicity. The gain/bandwidth control elements C g and R g are typically 10μF to 1500μF and 10 Q to 100Q respectively. The values chosen for C g and R g set f c , the 3dB cut-off frequency, and a typical value for this in the above techniques is 0.14Hz. The differential gain is determined by Rf and R g and the noise 1s related to the differential gain. Values of Rf above 1MΩ increase the noise significantly. A value of Rf around 300kΩ is a good compromise with C g at llOOμF and R g at 1 Ω. This enables the use of the minimum number of high-quality operational amplifiers while achieving high gain at low noise and resistance to interference from e.g. CRT scan frequencies and power freqencies such as 50 Hz, 60 Hz and their harmonics. The front end (FE) is connected to a receiver (R) by a signal line SL of up to three to five meters. The receiver also includes a regulated power supply (PSU) which supplies DC power to the receiver and via a similar length of power line PL, the front end where a DC/DC convertor provides appropriate voltages. The receiver channel output, for example Ch X, is connected to a high pass filter. The receiver gain is adjustable with a gain trim GT. The rest of the components and values are shown in Figure 11. Screened and balanced cables are used as indicated. Constructional details appropriate to the high-gain, low-noise requirements will be apparent to those skilled in the art. Clearly variations are possible for specific components and applications. Other equipment than that specifically described may be used to carry out the techniques of the invention, having regard to the performance requirement set out above.

Claims: CLAIMS 1. A method of analysing Ventricular Late Potential (VLP) including determining a parameter related to the complexity of the VLP as a a parameter for clinical evaluation. 2. A method of analysing Ventricular Late Potential (VLP) including computing the fractal dimension of the attractor for the VLP as a parameter for clinical evaluation. 3. A method according to Claim 2 including computing the VLP attractor fractal dimension in three dimensional voltage space, the voltage being ECG measurements. 4. A method according to Claim 3 including providing an approximation to the fractal dimension of the attractor as the quotient of log(L)/log(DD), where L is the total length of the attractor and DD is the spheric extent of the attractor. 5. A method according to Claim 3 including assessing the ECG signals to define VLP onset and offset points. 6. A method according to Claim 5 including assessing the ECG signals by signal-averaging and high-pass filtering and taking the absolute value of the filtered output. 7. A method according to Claim 5 including defining the onset point as the vector magnitude combination exceeding one of a chosen mean and a chosen peak voltage. 8. A method according to Claim 7 including choosing the vector magnitude as one of 40 micro volts mean and 48 microvolts peak (mean ± 20%). 9. A method according to Claim 5 including defining the offset point as the mean voltage exceeding the mean noise level plus three times the standard deviation of the noise sample. 10. A method according to Claim 2 including providing a specific output on computing a fractal dimension in excess of a value selected as the value indicating a risk of sudden cardiac death positive (SCD+) condition. 11. A method according to Claim 10 including selecting the value as a fractal dimension in excess of 1.30. 12. A method according to Claim 2 including collecting ECG signal with an amplifier having three operational amplifiers with a high gain in an early front end stage arranged to minimise noise over a controlled bandwidth of 0.1 to 1200Hz and reduce crosstalk below -90dB. 13. A method of analysing Ventricular Late Potential including performing a spectral analysis producing an assessment based on a discrete Hartley transform (DHT) vector spectrum by summing amplitude components between -f^ to -f 2 and +f 2 to +f ] , where f ] is a number larger than f 2 . 14. A method according to Claim 13 including identifying for a group including persons believed healthy and persons believed to be SCD+ a value in the upper part of the range of individual assessments as indicating risk of SCD+. 15. A method according to Claim 4 including producing the approximation by the application of an algorithm. 16. A method according to Claim 15 including applying the algorithm in the form of a flow chart. 17. An apparatus to analyse Ventricular Late Potential (VLP) including means to receive VLP signals and means to compute the fractal dimension of the attractor for the VLP as a parameter for clinical evaluation. 18. An apparatus according to Claim 17 including means to compute the VLP attractor for three dimensional voltage space, the voltage being ECG measurements. 19. An apparatus according to Claim 17 including means to receive ECG signals having signal channel amplifiers including three operational amplifierswith a high gain in a front end stage over a controlled bandwidth and reduced crosstalk. 20. An apparatus according to Claim 19 in which the bandwidth is 0.1 Hz to 1200 Hz and the crosstalk below -90db. 21. Apparatus according to Claim 17 including ECG signal-averaging means and high-pass filtering means and means to deliver the absolute value of the filtered output. 22. Apparatus according to Claim 16 including means to provide an appropriate output indication on the determination of a parameter value in excess of, or below, a selected value.

Inventors: ESCALONA OMAR JACINTO, ESCALONA, OMAR, JACINTO
Applicants: BRITISH TECH GROUP, ESCALONA OMAR JACINTO, BRITISH TECHNOLOGY GROUP LIMITED, ESCALONA, OMAR, JACINTO
Application year: 1994
Main classification: G06F15
IPC codes: A61B5, G06F17, G06Q50